Physics Notes - Herong's Tutorial Notes - v3.24, by Herong Yang
Motion Equations of Linear Systems
This section provides a quick introduction of motion equations of linear systems, which are first order linear differential equations of the canonical coordinates.
What Is Linear System? A Linear System is a system where motion equations are first order linear differential equations of the canonical coordinates. In this case, motion equations can be expressed in the vector form as shown below:
x' = Ax + b (P.12) where: x is the vector of [q1, q2, ..., p1, p2, ....] x' is the vector of dx/dt A is a matrix of coefficients b is a constant vector
For a Linear System of a single object with 1 degree of freedom, vector x is [q, p] and x' is [q', p']. The motion equations can be expressed as:
|q'| = |a11, a12| . |q| + |b1| |p'| |a21, a22| |p| |b2|
Now let's look at those systems of motions presented earlier:
1. The Free Fall Motion of a single object is a linear system. The motion equations can be expressed as:
m*g = -p' (P.4) p/m = q' (P.5) In vector form: |q'| = |0, 1/m| . |q| + | 0| |p'| |0, 0| |p| |-m*g|
2. An object on a spring moving horizontally is a linear system. The motion equations can be expressed as:
kq = -p' (P.7) p/m = q' (P.8) In vector form: |q'| = | 0, 1/m| . |q| + |0| |p'| |-k, 0| |p| |0|
3. A simple pendulum is not a linear system, because p' is not linearly related to q:
m*g*l*sin(q) = -p' (P.10) p/(m*l*l) = q' (P.11)
Table of Contents
Introduction of Frame of Reference
Introduction of Special Relativity
Time Dilation in Special Relativity
Length Contraction in Special Relativity
The Relativity of Simultaneity
Minkowski Spacetime and Diagrams
Introduction of Generalized Coordinates
►Phase Space and Phase Portrait
Phase Portrait of Simple Harmonic Motion
Phase Portrait of Pendulum Motion
►Motion Equations of Linear Systems